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PILE FOUNDATION.
One or more of the followings:
(a)Transfer load to stratum of adequate capacity
(b)Resist lateral loads.
(c)1
Transfer loads through a scour zone to bearing stratum
(d)Anchor structures subjected to hydrostatic uplift or overturning
s
Pile
pQ
Q
uQ
spu QQQ +=
1
Check setlements of pile groups
R. KHERA 1 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Do not use piles if:
Driving may cause damage to adjacent structures, soil may heave
excessively, or in boulder fields.
Pile Installation
Hammers
Drop hammer1
Pile
Pile cap
Cushion
Ram
Drop hammer
Cushion
1
Very noisy, simple to operate and maintain , 5-10 blows / minute, slow driving, very large drop, not suited for end bearing piles,
used on Franki piles
R. KHERA 2 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Exhaust
Intake
Ram
Pile cap
Cushion
Pile
Single acting hammer
Cushion
Double acting1
:
Differential acting2
Diesel3
Vibratory4
Jacking
Predrilling or Jetting
1
Uses pressure for up stroke and down stroke. Design limits prevent it to deliver as much energy as single acting, but greater speed,
used mostly for sheet piles
2
Has two pistons with different diameters, allowing it to have heavy ram as for single acting and greater speed as double acting
3
Difficult to drive in soft ground, develops max energy in hard driving
4
Rotating eccentric loads cause vertical vibrations, most effective in sand
R. KHERA 3 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
PILE TYPE
• Timber
• Concrete
• Steel
Timber piles
Butt dia 12" to 20", tip 5" to 10". Length 30-60'
Bark always removed.
Concrete piles
Pre-cast
• Reinforce and prestressed
Cast in place
• With or without casing1
• More common than precast.
Steel Piles
• Steel H-Pile
• Unspliced 140', spliced > 230', load 40 to 120 tons.
1
more economical but more risk in their installation .
R. KHERA 4 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
PILES CLASSIFICATION
1. Material (wood, steel, etc.).
2. Method of installation1
3. Effect on surrounding soils during installation2
.
Pile load capacity prediction
• Full-scale load test
• Static formulae
• Dynamic method
1
(driven: blow of a hammer, vibrations, pressure from a jack, etc.; jetted, augured, screwing, etc.).
2
displacement, non-displacement
R. KHERA 5 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Pile shape effect and pile selection
Shape
characteristics
Pile type placement effect
Displacement Closed ended steel Increase lateral ground stress
Precast concrete Densifies granular soils,
weakens clays1
Tapered Timber,
monotube, thin-
walled shell
High capacity for short
length in granular soils
Non-
displacement
Steel H Minimal disturbance to soil
Open ended steel
pipe
Not suitable for friction piles
in granular soils, often show
low driving resistance, field
varification difficult
resulting in excessive pile
length
1
Seup time for large groups upto 6-months
R. KHERA 6 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Load Transfer
s
D
Pile
pQ
L Q
uQ
soil plug
Ap = total plan area
steel
steel
q'
soil plug
Q Q Qu p s= +
Settlement for full load transfer
• Qp →0.1D (driven), 0.25 D (bored)
• Qs →0.2" - 0.3"
R. KHERA 7 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
End or Point Resistance
qult = cN*c + q'oN*q + γDN*γ
D = pile diameter or width
q'o = effective overburden stress at pile tip
N*c, N*q,N*γ are the b.c. factors which include shape and depth
factors
Since pile dia is small γDN*γ ≈ 0
)NqcN(AQ *
q
'
o
*
cpp +=
Ap = pile tip area
R. KHERA 8 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Meyerhof's Method
Point resistance increases with depth reaching a maximum value at
Lb/D critical.
(Lb/D)crit varies with φ and c. Fig 9.12
Lb = embedment length in bearing soil
D
L
Qp
L/D
(L/D)cri
For values of N*c, N*q see Fig 9.13
R. KHERA 9 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Piles in Sand1
Q A q N Ap p o
'
q
*
p= ⋅ ⋅ ≤ q⋅ l
where q φ⋅= tan0.5N(tsf) *
ql
φ in terms of 'N' or Dr
o
15N20 +=φ
r
o
D1528 +=φ
Point resistance from SPT
N4
D
LN0.4
=(tsf)qp ⋅≤
⋅⋅
N = avg value for 10D above and 4D below pile tip
10D
4D
Q
1
For a given initial φ unit point resistance for bored piles =1/3 to 1/2 of driven piles, and bulbous piles driven with great impact
energy have upto about twice the unit resistance of driven piles of constant section
R. KHERA 10 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Example 1
A pile with L = 65', x-section = 18"×18" is embedded in sand with
φ = 30°, γ = 118.3 pcf. Estimate point bearing resistance.
Solution (Meyerhof)
Q A q N Ap p o
'
q
*
p= ⋅ ⋅ ≤ q⋅ l
tons47620005565118.35.15.1Qp =÷××××=
tons36tan30550.51.51.5qAQ lpp =××××=⋅=
R. KHERA 11 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Upper weak lower firm soil
Lb
L
dense
sand
q l(d)
10D
q
l(l)
loose
sand
( ) l(d)l(l)l(d)
b
l(l)p qqq
10D
L
qq ≤−+=
ql(l) = limiting point resistance in loose sand
ql(d) = limiting point resistance in dense sand
Piles in Saturated Clay
If embedded length ≥ 5D, Nc
*
= 9
pup Ac9Q ⋅⋅=
R. KHERA 12 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Example 2
Timber piles, 25' log with 10" point diameter, were driven through
a silty sand with φ = 25° into undrelying dense sandy gravel with φ
= 40°. Penetration into the sandy gravel was 3'. Determine point
bearing capacity of a pile.
Solution
ql (silty sand) = 0.5Nq
*
tan φ = 0.5×25 tan 25 = 5.82 tsf
ql (sandy gravel) = 0.5×350× tan 40 = 146.8 tsf
( ) 8.461tsf6.5682.58.461
1010
36
82.5qp <=−
×
+=
tons30.956.6
212
10
Q
2
p =×π×





×
=
R. KHERA 13 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Shaft Resistance
It is due to skin friction and adhesion
sAfQs ⋅Σ=
As = area of shaft surface
f = unit shaft resistance
z
L
L'
K
f
D
σ
v
'
f
aoK ctanf '
+= δσ
δ = soil-pile friction angle
ca = is adhesion
K = earth pressure coefficient1
1
which is difficult to evaluate between at-rest and passive state
R. KHERA 14 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Shaft Resistance in Sand
Since ca= 0
δσ tanKf '
⋅⋅= o
Like tip resistance a critical depth is reached after which 'f' does not
increase. Use (L'/D)critical =15
Values of K
Pile type K
Bored or jetted Ko = 1 - sin φ
low disp. driven Ko to 1.4 Ko
high disp. driven Ko to 1.8 Ko or
0.5 +0.008 Dr
1
1
Dr = relative density (%)
R. KHERA 15 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Pile material δ
steel 20°
concrete 0.75 φ
wood 0.67φ
LfpQs ∆⋅⋅Σ=
p = perimeter
∆L = incremental pile length for constant p and f.
R. KHERA 16 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
SPT - basis for shaft resistance in sand
Meyerhof
50
N
=(tsf)favg high disp. driven piles
100
N
=(tsf)favg small disp. driven (H-pile)
50
N
1.5=(tsf)favg ⋅ pile tapered > 1%
N avg 'N' within embedded pile length=
R. KHERA 17 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Skin Resistance in Clay1
λ Method2
( )u
'
vav 2cf +σλ=
σ v
'
= mean effective vertical stress on pile length
λ- given in Fig. 8.17
LfpQ avs ⋅⋅=
For layered soils use mean values of cu and σ.
C2
C3
L3
L1
L L2 Cu
C1C1
'σ
A3
C v
A2
'σv
A1
L
...+Lc+Lc
=c 2u(2)1u(1)
u
1
some problems 1. increase in pore water pressure 2. Low initial capacity 3. enlarged hole near ground surface-water may get in and
soften clay. 4.ground and pile heaving. 5. Drag down effect from soft upper soils
2
Short pile were driven in stiff clay OCR>1 but the long piles penetrated lower soft clay as well
R. KHERA 18 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
L
....AAA 321'
v
+++
=σ
A1, A2, ... are areas of the effective stress diagrams
R. KHERA 19 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Example 3
A 12 m prestressed concrete pile 450 mm square is installed in a
clay with water table at 5 m depth. Upper clay layer is 5 m thick,
with γ = 17.4 kN/m3
and cu = 50 kPa. Lower clay has γ = 18.1
kN/m3
, cu = 75 kPa. Determine pile capacity using λ - method.
Solution: (λ - method)
'cu
5m
7m
87 kPa75 kPa
145 kPa
vσ
50 kPa
σ5
'
= 17.4×5 = 87 kPa, σ12
'
= 87 + (18.1-9.81)×7 = 145 kPa
64.58kPa
12
775550
cu =
×+×
=
85.79kPa
12
2
14587
75870.5
'
v =
+
×+××
=σ
R. KHERA 20 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
σcu
64.58 kPa 85.79 kPa
'v-avg
1
λ = 0.24
favg = 0.24(85.79+2×64.58) = 51.6 kPa
Qs = 4×0.45×51.6×12 = 1114 kN
1
Fig 9.17
R. KHERA 21 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Example 4. Redo Example 3 using α - method
ucFf ⋅⋅= α
Upper clay, 57.0
87
50c
'
u
==
oσ
cu/σ
α
0.570.35 0.8
0.5
1.0
756.0)57.08.0(
35.08.0
5.01
5.0 =−
−
−
+=α
L/D = 12/0.45 = 26.7, F = 1
Lower clay
517.0
145
75c
'
u
==
oσ
α = 0.814,
f1 = 1×0.756×50 = 37.8 kPa
f2 = 1×0.814×75 = 61.05 kPa
Qs = 4×0.45×5×37.8 +4×0.45×7×61.05 = 1109 kN
R. KHERA 22 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Example 5. Redo the Example 3 assuming 200 mm pipe
L/D = 12/0.2 = 60
L/D
1.0
F
6050 120
0.7
( )( )
0.95
50120
601200.71
0.7F =
−
−−
+=
f1 = 0.95×0.756×50 = 35.9 kPa
f2 = 0.95×0.814×75 = 58.0 kPa
Qs = π(0.2) × (5×35.9 +7×58.0) = 368 kN
R. KHERA 23 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Example 6
Draw number of blows per inch versus Ru for the following
conditions using EN formula, modified Engineering News formula,
and Janbu formula. Steel HP10×57, coefficient of restitution (n) =
0.8, efficiency (E) = 0.85, Vulcan 08 hammer. C = 0.1". 1
Use two
pile lengths 20' and 80'. Elastic modulus = 29×103
ksi
Solution
Hammer energy 26 k-ft, Ram weight 8 kips. Area of steel = 16.8
in2
.
C 0.75 0.15
57 20
8000
d = +
×
= 0 771.
Assume S = 0.1"
( )
06.13
1.010298.16
26122085.
23
=
×××
×××
=λ
382.40
0.771
06.13
11771.0Ku =





++=
Ru (20 ft for S=0.1") = 657 kips
Ru (80 ft for S=0.1") = 354 kips
1
For plotting graphs assume several Ru and compute set
R. KHERA 24 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Bearing Graph
Ru - Janbu 20', Ru1 - Janbu 80', Rmn = Modified EN 20', Rmn1 =
Modified EN 80'
From Modified Engineering New Formula, the following results
will be obtained.
Ru (20 ft for S=0.1") = 1266 kips
Ru (80 ft for S=0.1") = 1153 kips
R. KHERA 25 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Practical applications
Design
• Using laboratory and field soil data determine Qu based on static
formulae
Test pile
• Drive test piles using same equipment as proposed for
production piles.
• If possible use pile driving analyser (PDA) incorporating strain
and acceleration data on test pile. Prepare bearing graph.
• Make records of pile driving and correlate with boring logs to
ensure that piles have penetrated the bearing soils.
• Load test the pile/s.
• If possible load to failure to establish actual factor safety.
• For small jobs load tests are not justifiable.
• When piles rest on sound bedrock load tests may not be
necessary.
• Based on load test adjust design capacity, increase penetration
depth, alter driving criteria as necessary.
Construction stage
• Record driving resistance for full depth of penetration
• Driving record must correspond to bearing graph of test pile.
R. KHERA 26 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
• If not additional penetration into bearing material or greater
driving resistance may be necessary.
R. KHERA 27 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Wave Equation
• Hammer, cushions, pile cap, and pile are modeled as discrete
elements.
• Each element has a mass and there are springs between element
of appropriate stiffness
• Soil-pile interface modeled as spring-dash pot. Springs model
resistance to driving as a function of displacement and dash pots
as function of velocity.
Computations
• Ram of mass M1 with velocity v1 travels a distance v1×∆t
compresses spring K1 with the same amount.
• Force in K1 actuates M2 from which displacements are
computed.
• Process is continued for all masses for successive time intervals
until pile tip stops moving.
• Software - TTI and WEAP (Wave Equation Analysis of Pile)
R. KHERA 28 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
R. KHERA 29 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
Pile Driving Analyser
• Two strain transducers and two accelerometers mounted near
pile head
• A pile driving analyser (PDA)
PDA monitors strain and acceleration and yields:
• Force in pile - from strain, E and pile x-sectopm
• Particle velocity - from integration of acceleration
• Pile set - from integration of velocity
CAPWAP(Case Pile Wave Analysis Program):
Hammer and accessories - replaced by force-time and velocity-time
time data from PDA, thus eliminating deficiencies of wave
equation.

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Pile exmplsolu

  • 1. PILE FOUNDATION. One or more of the followings: (a)Transfer load to stratum of adequate capacity (b)Resist lateral loads. (c)1 Transfer loads through a scour zone to bearing stratum (d)Anchor structures subjected to hydrostatic uplift or overturning s Pile pQ Q uQ spu QQQ += 1 Check setlements of pile groups R. KHERA 1 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 2. Do not use piles if: Driving may cause damage to adjacent structures, soil may heave excessively, or in boulder fields. Pile Installation Hammers Drop hammer1 Pile Pile cap Cushion Ram Drop hammer Cushion 1 Very noisy, simple to operate and maintain , 5-10 blows / minute, slow driving, very large drop, not suited for end bearing piles, used on Franki piles R. KHERA 2 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 3. Exhaust Intake Ram Pile cap Cushion Pile Single acting hammer Cushion Double acting1 : Differential acting2 Diesel3 Vibratory4 Jacking Predrilling or Jetting 1 Uses pressure for up stroke and down stroke. Design limits prevent it to deliver as much energy as single acting, but greater speed, used mostly for sheet piles 2 Has two pistons with different diameters, allowing it to have heavy ram as for single acting and greater speed as double acting 3 Difficult to drive in soft ground, develops max energy in hard driving 4 Rotating eccentric loads cause vertical vibrations, most effective in sand R. KHERA 3 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 4. PILE TYPE • Timber • Concrete • Steel Timber piles Butt dia 12" to 20", tip 5" to 10". Length 30-60' Bark always removed. Concrete piles Pre-cast • Reinforce and prestressed Cast in place • With or without casing1 • More common than precast. Steel Piles • Steel H-Pile • Unspliced 140', spliced > 230', load 40 to 120 tons. 1 more economical but more risk in their installation . R. KHERA 4 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 5. PILES CLASSIFICATION 1. Material (wood, steel, etc.). 2. Method of installation1 3. Effect on surrounding soils during installation2 . Pile load capacity prediction • Full-scale load test • Static formulae • Dynamic method 1 (driven: blow of a hammer, vibrations, pressure from a jack, etc.; jetted, augured, screwing, etc.). 2 displacement, non-displacement R. KHERA 5 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 6. Pile shape effect and pile selection Shape characteristics Pile type placement effect Displacement Closed ended steel Increase lateral ground stress Precast concrete Densifies granular soils, weakens clays1 Tapered Timber, monotube, thin- walled shell High capacity for short length in granular soils Non- displacement Steel H Minimal disturbance to soil Open ended steel pipe Not suitable for friction piles in granular soils, often show low driving resistance, field varification difficult resulting in excessive pile length 1 Seup time for large groups upto 6-months R. KHERA 6 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 7. Load Transfer s D Pile pQ L Q uQ soil plug Ap = total plan area steel steel q' soil plug Q Q Qu p s= + Settlement for full load transfer • Qp →0.1D (driven), 0.25 D (bored) • Qs →0.2" - 0.3" R. KHERA 7 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 8. End or Point Resistance qult = cN*c + q'oN*q + γDN*γ D = pile diameter or width q'o = effective overburden stress at pile tip N*c, N*q,N*γ are the b.c. factors which include shape and depth factors Since pile dia is small γDN*γ ≈ 0 )NqcN(AQ * q ' o * cpp += Ap = pile tip area R. KHERA 8 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 9. Meyerhof's Method Point resistance increases with depth reaching a maximum value at Lb/D critical. (Lb/D)crit varies with φ and c. Fig 9.12 Lb = embedment length in bearing soil D L Qp L/D (L/D)cri For values of N*c, N*q see Fig 9.13 R. KHERA 9 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 10. Piles in Sand1 Q A q N Ap p o ' q * p= ⋅ ⋅ ≤ q⋅ l where q φ⋅= tan0.5N(tsf) * ql φ in terms of 'N' or Dr o 15N20 +=φ r o D1528 +=φ Point resistance from SPT N4 D LN0.4 =(tsf)qp ⋅≤ ⋅⋅ N = avg value for 10D above and 4D below pile tip 10D 4D Q 1 For a given initial φ unit point resistance for bored piles =1/3 to 1/2 of driven piles, and bulbous piles driven with great impact energy have upto about twice the unit resistance of driven piles of constant section R. KHERA 10 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 11. Example 1 A pile with L = 65', x-section = 18"×18" is embedded in sand with φ = 30°, γ = 118.3 pcf. Estimate point bearing resistance. Solution (Meyerhof) Q A q N Ap p o ' q * p= ⋅ ⋅ ≤ q⋅ l tons47620005565118.35.15.1Qp =÷××××= tons36tan30550.51.51.5qAQ lpp =××××=⋅= R. KHERA 11 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 12. Upper weak lower firm soil Lb L dense sand q l(d) 10D q l(l) loose sand ( ) l(d)l(l)l(d) b l(l)p qqq 10D L qq ≤−+= ql(l) = limiting point resistance in loose sand ql(d) = limiting point resistance in dense sand Piles in Saturated Clay If embedded length ≥ 5D, Nc * = 9 pup Ac9Q ⋅⋅= R. KHERA 12 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 13. Example 2 Timber piles, 25' log with 10" point diameter, were driven through a silty sand with φ = 25° into undrelying dense sandy gravel with φ = 40°. Penetration into the sandy gravel was 3'. Determine point bearing capacity of a pile. Solution ql (silty sand) = 0.5Nq * tan φ = 0.5×25 tan 25 = 5.82 tsf ql (sandy gravel) = 0.5×350× tan 40 = 146.8 tsf ( ) 8.461tsf6.5682.58.461 1010 36 82.5qp <=− × += tons30.956.6 212 10 Q 2 p =×π×      × = R. KHERA 13 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 14. Shaft Resistance It is due to skin friction and adhesion sAfQs ⋅Σ= As = area of shaft surface f = unit shaft resistance z L L' K f D σ v ' f aoK ctanf ' += δσ δ = soil-pile friction angle ca = is adhesion K = earth pressure coefficient1 1 which is difficult to evaluate between at-rest and passive state R. KHERA 14 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 15. Shaft Resistance in Sand Since ca= 0 δσ tanKf ' ⋅⋅= o Like tip resistance a critical depth is reached after which 'f' does not increase. Use (L'/D)critical =15 Values of K Pile type K Bored or jetted Ko = 1 - sin φ low disp. driven Ko to 1.4 Ko high disp. driven Ko to 1.8 Ko or 0.5 +0.008 Dr 1 1 Dr = relative density (%) R. KHERA 15 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 16. Pile material δ steel 20° concrete 0.75 φ wood 0.67φ LfpQs ∆⋅⋅Σ= p = perimeter ∆L = incremental pile length for constant p and f. R. KHERA 16 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 17. SPT - basis for shaft resistance in sand Meyerhof 50 N =(tsf)favg high disp. driven piles 100 N =(tsf)favg small disp. driven (H-pile) 50 N 1.5=(tsf)favg ⋅ pile tapered > 1% N avg 'N' within embedded pile length= R. KHERA 17 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 18. Skin Resistance in Clay1 λ Method2 ( )u ' vav 2cf +σλ= σ v ' = mean effective vertical stress on pile length λ- given in Fig. 8.17 LfpQ avs ⋅⋅= For layered soils use mean values of cu and σ. C2 C3 L3 L1 L L2 Cu C1C1 'σ A3 C v A2 'σv A1 L ...+Lc+Lc =c 2u(2)1u(1) u 1 some problems 1. increase in pore water pressure 2. Low initial capacity 3. enlarged hole near ground surface-water may get in and soften clay. 4.ground and pile heaving. 5. Drag down effect from soft upper soils 2 Short pile were driven in stiff clay OCR>1 but the long piles penetrated lower soft clay as well R. KHERA 18 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 19. L ....AAA 321' v +++ =σ A1, A2, ... are areas of the effective stress diagrams R. KHERA 19 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 20. Example 3 A 12 m prestressed concrete pile 450 mm square is installed in a clay with water table at 5 m depth. Upper clay layer is 5 m thick, with γ = 17.4 kN/m3 and cu = 50 kPa. Lower clay has γ = 18.1 kN/m3 , cu = 75 kPa. Determine pile capacity using λ - method. Solution: (λ - method) 'cu 5m 7m 87 kPa75 kPa 145 kPa vσ 50 kPa σ5 ' = 17.4×5 = 87 kPa, σ12 ' = 87 + (18.1-9.81)×7 = 145 kPa 64.58kPa 12 775550 cu = ×+× = 85.79kPa 12 2 14587 75870.5 ' v = + ×+×× =σ R. KHERA 20 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 21. σcu 64.58 kPa 85.79 kPa 'v-avg 1 λ = 0.24 favg = 0.24(85.79+2×64.58) = 51.6 kPa Qs = 4×0.45×51.6×12 = 1114 kN 1 Fig 9.17 R. KHERA 21 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 22. Example 4. Redo Example 3 using α - method ucFf ⋅⋅= α Upper clay, 57.0 87 50c ' u == oσ cu/σ α 0.570.35 0.8 0.5 1.0 756.0)57.08.0( 35.08.0 5.01 5.0 =− − − +=α L/D = 12/0.45 = 26.7, F = 1 Lower clay 517.0 145 75c ' u == oσ α = 0.814, f1 = 1×0.756×50 = 37.8 kPa f2 = 1×0.814×75 = 61.05 kPa Qs = 4×0.45×5×37.8 +4×0.45×7×61.05 = 1109 kN R. KHERA 22 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 23. Example 5. Redo the Example 3 assuming 200 mm pipe L/D = 12/0.2 = 60 L/D 1.0 F 6050 120 0.7 ( )( ) 0.95 50120 601200.71 0.7F = − −− += f1 = 0.95×0.756×50 = 35.9 kPa f2 = 0.95×0.814×75 = 58.0 kPa Qs = π(0.2) × (5×35.9 +7×58.0) = 368 kN R. KHERA 23 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 24. Example 6 Draw number of blows per inch versus Ru for the following conditions using EN formula, modified Engineering News formula, and Janbu formula. Steel HP10×57, coefficient of restitution (n) = 0.8, efficiency (E) = 0.85, Vulcan 08 hammer. C = 0.1". 1 Use two pile lengths 20' and 80'. Elastic modulus = 29×103 ksi Solution Hammer energy 26 k-ft, Ram weight 8 kips. Area of steel = 16.8 in2 . C 0.75 0.15 57 20 8000 d = + × = 0 771. Assume S = 0.1" ( ) 06.13 1.010298.16 26122085. 23 = ××× ××× =λ 382.40 0.771 06.13 11771.0Ku =      ++= Ru (20 ft for S=0.1") = 657 kips Ru (80 ft for S=0.1") = 354 kips 1 For plotting graphs assume several Ru and compute set R. KHERA 24 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 25. Bearing Graph Ru - Janbu 20', Ru1 - Janbu 80', Rmn = Modified EN 20', Rmn1 = Modified EN 80' From Modified Engineering New Formula, the following results will be obtained. Ru (20 ft for S=0.1") = 1266 kips Ru (80 ft for S=0.1") = 1153 kips R. KHERA 25 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 26. Practical applications Design • Using laboratory and field soil data determine Qu based on static formulae Test pile • Drive test piles using same equipment as proposed for production piles. • If possible use pile driving analyser (PDA) incorporating strain and acceleration data on test pile. Prepare bearing graph. • Make records of pile driving and correlate with boring logs to ensure that piles have penetrated the bearing soils. • Load test the pile/s. • If possible load to failure to establish actual factor safety. • For small jobs load tests are not justifiable. • When piles rest on sound bedrock load tests may not be necessary. • Based on load test adjust design capacity, increase penetration depth, alter driving criteria as necessary. Construction stage • Record driving resistance for full depth of penetration • Driving record must correspond to bearing graph of test pile. R. KHERA 26 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 27. • If not additional penetration into bearing material or greater driving resistance may be necessary. R. KHERA 27 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 28. Wave Equation • Hammer, cushions, pile cap, and pile are modeled as discrete elements. • Each element has a mass and there are springs between element of appropriate stiffness • Soil-pile interface modeled as spring-dash pot. Springs model resistance to driving as a function of displacement and dash pots as function of velocity. Computations • Ram of mass M1 with velocity v1 travels a distance v1×∆t compresses spring K1 with the same amount. • Force in K1 actuates M2 from which displacements are computed. • Process is continued for all masses for successive time intervals until pile tip stops moving. • Software - TTI and WEAP (Wave Equation Analysis of Pile) R. KHERA 28 PileExmplSolu.doc04/14/03 PileExmplSolu.doc
  • 29. R. KHERA 29 PileExmplSolu.doc04/14/03 PileExmplSolu.doc Pile Driving Analyser • Two strain transducers and two accelerometers mounted near pile head • A pile driving analyser (PDA) PDA monitors strain and acceleration and yields: • Force in pile - from strain, E and pile x-sectopm • Particle velocity - from integration of acceleration • Pile set - from integration of velocity CAPWAP(Case Pile Wave Analysis Program): Hammer and accessories - replaced by force-time and velocity-time time data from PDA, thus eliminating deficiencies of wave equation.